An ultra low phase noise microwave synthesizer for providing an output signal having a frequency FO of from 2 GHz to 20 GHz using a first voltage controlled oscillator (vco), a first frequency comparing circuit for driving said first vco to a first selected frequency (Fidle), a first circuit including a first harmonic sampler for phase locking said first vco to said first selected frequency (Fidle), a second vco, a second frequency comparing circuit coupled to said first vco for driving said second vco to a second selected frequency (Fcoarse), a second circuit coupled to said first vco including a second harmonic sampler for phase locking said second vco to said second selected frequency (Fcoarse), a third vco, and a third circuit coupled to said second vco including a third harmonic sampler for phase locking said third vco to said frequency FO.
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1. An ultra low phase noise microwave synthesizer for providing an output signal having a frequency FO comprising:
a first voltage controlled oscillator (vco); first frequency comparing means for driving said first vco to a first selected frequency (Fidle); first means including a first harmonic sampler for phase locking said first vco to said first selected frequency (Fidle); a second vco; second frequency comparing means coupled to said first vco for driving said second vco to a second selected frequency (Fcoarse); second means coupled to said first vco including a second harmonic sampler for phase locking said second vco to said second selected frequency (Fcoarse); a third vco; and third means coupled to said second vco including a third harmonic sampler for phase locking said third vco to said frequency FO.
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15. A synthesizer according to
an oscillator having a predetermined frequency; a first multiplier responsive to said predetermined frequency for providing said first selected reference frequency Fref1 ; a second multiplier responsive to said predetermined frequency for providing said second selected reference frequency Fref2 ; and a mixer responsive to said first selected reference frequency Fref1 if the second selected frequency (Fcoarse) is greater than or equal to a predetermined frequency or said second selected reference frequency Fref2 if the second selected frequency (Fcoarse) is less than said predetermined frequency and said second selected frequency (Fcoarse) for providing said frequency (FD) .
16. A synthesizer according to
means for inverting the signal applied to the voltage control input of the second vco when the second selected frequency (Fcoarse) is greater than or equal to a predetermined frequency.
17. A synthesizer according to
18. A synthesizer according to
a programmable divider for providing an output signal having a frequency FS which is a fraction 1/P of the second selected frequency Fcoarse ; means including said third harmonic sampler for sampling the output of said third vco at said frequency FS for providing an error signal; and means, including a means for detecting the phase difference between a signal having a reference frequency Ffine and said error signal, for providing a control voltage for controlling the frequency FO of said third vco.
19. A synthesizer according to
20. A synthesizer according to
21. A synthesizer according to
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1. Field of the Invention
The present invention relates to microwave synthesizers in general and in particular to a method and apparatus comprising a means for eliminating digital divider noise in conjunction with a topology that reduces the harmonic number used in the synthesis of microwave signals.
2. Description of the Related Art
A microwave synthesizer is a circuit which is used for generating microwave signals of any frequency within a predetermined, generally broad, range of frequencies.
Heretofore, noise performance pertaining to synthesized microwave signal generation, in particular sources that must produce any frequency, such as a synthesizer, has been limited by digital divider noise and the multiplying nature of harmonic samplers increasing this noise by the harmonic number H. For example, the output frequency of prior known synthesizers can be represented by the following equation ##EQU1## wherein the frequency Fstep, i.e. the midrange frequency, is multiplied by the harmonic number H.
In view of the foregoing, a principal object of the present invention is an ultra low phase noise microwave frequency synthesizer wherein digital divider noise is eliminated in conjunction with a topology that reduces the harmonic number used in the synthesis of microwave signals. Furthermore, the midrange frequency is no longer multiplied by the harmonic number H and the output frequency FO is given by an equation of the following form: ##EQU2##
The synthesizer of the present invention is usable in a variety of applications, such as, for example, the front end of a spectrum analyzer.
In accordance with the above, there is provided a synthesizer comprising essentially three stages. In the first stage there is provided a circuit responsive to a reference frequency Fstep and a control signal corresponding to a frequency Fidle for providing the frequency Fidle. In the second stage there is provided a circuit responsive to the frequency Fidle, a selected one of a pair of reference frequencies Fref1 and Fref2, and a control signal corresponding to a frequency Fcoarse, control signals for selecting between Fref1 and Fref2 and a control signal for controlling a polarity circuit for providing the frequency Fcoarse. In the third stage there is provided a circuit responsive to Fcoarse, a reference frequency Ffine, and a plurality of control signals for controlling a programmable divider, the frequency Ffine and a polarity circuit for providing an output signal having a frequency FO given by an equation of the following general form: ##EQU3##
In the circuit providing the frequency Fidle there is provided a first harmonic sampler, a first programmable frequency presteer circuit, a first summing circuit and a first VCO. The frequency Fidle is a selected multiple of the frequency Fstep.
In operation, the control signal corresponding to the frequency Fidle is applied to the first presteer circuit for driving the first VCO via the first summing circuit to the selected frequency Fidle. When the first VCO is at Fidle, the output of the first presteer circuit is rendered null and the first sampler takes over to phase-lock the first VCO via the first summing circuit to the selected frequency Fidle.
In the circuit providing the frequency Fcoarse there is provided a second harmonic sampler, a second programmable frequency presteer circuit, a second summing circuit and a second VCO, a polarity circuit, a mixer and a source of two reference frequencies Fref1 and Fref2.
In operation, the control signal corresponding to the selected frequency Fcoarse is applied to the second presteer circuit for driving the second VCO via the summing circuit to the selected frequency Fcoarse. When the second VCO is at Fcoarse, the output of the second presteer circuit is rendered null and the second sampler takes over to phase-lock the second VCO via the second summing circuit to the selected frequency Fcoarse. The polarity circuit, mixer and reference frequencies Fref1 and Fref2 are used to provide a relatively low sampling frequency having a corresponding noise floor while providing Fcoarse at a relatively high frequency so as to minimize the harmonic number H in the circuit providing the output signal.
In the circuit providing the output signal having the frequency FO there is provided a programmable divider, a third harmonic sampler, a phase detector, a source of a reference frequency Ffine, a polarity circuit and a third VCO.
In operation, the programmable divider divides the 10 frequency Fcoarse by a selected factor which is then used to sample the output of the third VCO to provide an error signal relative to the reference frequency Ffine. The polarity circuit controls the polarity of the response of the third VCO to the error signal to provide the output signal having the frequency FO.
Among the important features of the present invention is the fact that the noise performance of the synthesizer of the present invention is at least 18.6 dBc/Hz better than prior known synthesizers operating over a comparable range of frequencies.
The above and other objects, features and advantages of the present invention will become apparent from the following detailed description of the accompanying drawings, in which:
FIG. 1 is a block diagram of a prior known frequency synthesizer;
FIG. 2 is a drawing of the noise performance of the synthesizer of FIG. 1;
FIG. 3 is a block diagram of a frequency synthesizer according to the present invention;
FIG. 4 is a drawing of the noise performance of the synthesizer of FIG. 3;
FIG. 5 is a block diagram of a multiplying circuit invented by applicant;
FIG. 6 is a block diagram of dividing circuit invented by applicant; and
FIG. 7 is a block diagram of a dividing circuit with frequency offset according to the present invention.
Referring to FIG. 1 there is illustrated a prior known frequency synthesizer designated generally as 1 for providing an output signal having a frequency FO in the range of 2 gigahertz (GHz) to 20 GHz. As seen in FIG. 2, the worst case noise performance of the circuit 1 is approximately -112 dBc/Hz at 2 GHz and -92 dBc/Hz at 20.5 GHz. The units dBc/Hz as used herein represent the single sideband (SSB) noise power in a one (1) Hz bandwidth offset from the carrier by 10 KHz.
In the synthesizer 1 there is provided an oscillator 2 comprising a frequency Fstep, e.g. 1 megahertz (MHz), coupled to an input of a phase detector 3 having a second input coupled to the output of a programmable divider 4. The divider 4 is programmed by a control signal N for dividing the frequency of its input signal by a factor of from 10 to 60 depending on the desired frequency FO. The output of the phase detector 3 is coupled to the control voltage input of a voltage-controlled oscillator (VCO) 5 by means of an operational amplifier 6 and an RC circuit 7 comprising a resistor R and a capacitor C. The output of the VCO 5 comprises a range of frequencies Fcoarse, e.g. 440 MHz to 490 MHz, and is coupled to a prescaler 10 and one input of a mixer 11. A second input of the mixer 11 is coupled to an oscillator 12 having a frequency Fref, e.g. 500 MHz. The output of the mixer 11 is coupled to an input of the divider 4.
The output of the prescaler 10 is provided to divide the frequency of its input signal by a predetermined factor, e.g. 2, and is coupled to the sampling input FS of a harmonic sampler 15. The output of the sampler 15 comprising an intermediate frequency FIF is coupled to one input of a phase detector 16. A second input of the phase detector 16 is coupled to the output of a tunable oscillator 17 which is adapted to provide an output having a range of frequencies Ffine, e.g. 8 MHz to 32 MHz depending on the desired frequency FO. The output of the phase detector 16 is coupled to a voltage control input of a VCO 18 by means of an operational amplifier 19. An RC circuit 20 comprising a resistor R and a capacitor C is coupled between the input and output of the amplifier 19. The output of the VCO 18 is coupled to the high frequency Fref input of the sampler 15 and provides the output signal having the synthesized frequency FO wherein ##EQU4##
As indicated above, the noise performance of apparatus used heretofore for synthesized microwave signal generation, in particular sources that have used conventional frequency dividers, have been limited by digital divider noise and the multiplying nature of harmonic samplers which heretofore has increased such noise by the harmonic number H of the sampler.
Digital divider noise has heretofore been a severely limiting factor in microwave circuits because of process dependent noise floors. For convenience, noise floors are defined herein in terms of noise power in connection with which the above-described units dBc/Hz are used. For example, in T2 L circuits which have a maximum operating frequency of approximately 100 megahertz (MHz), the noise floor is approximately -160 dBc/Hz. In Motorola emitter coupled logic (MECL) circuits which have a maximum operating frequency of approximately 600 MHz, the noise floor is approximately -150 dBc/Hz. In gallium-arsenide (GaAs) circuits, which have a maximum operating frequency of approximately 3000 MHz, i.e. 3 GHz, the noise floor is approximately -130 dBc/Hz. That is to say, each of the above-described circuits add the amount of noise indicated to the signal being processed therein.
To facilitate the following description of the noise performance of the prior art frequency synthesizer of FIG. 1, noise performance figures are provided for selected locations in the circuit. For example, the noise floor, i.e. noise power in the output, of the oscillator 2 which operates at 1 MHz is indicated as comprising -160 dBc/Hz, the noise floor of the oscillator 12 operating at 500 MHz is -150 dBc/Hz and the noise floor of the oscillator 17 operating at 8 MHz to 32 MHz is -160 dBc/Hz. For convenience and because of space limitations, the units dBc/Hz are abbreviated to dB in the drawings.
For purposes of the following description, a noise voltage level is defined by the following equation: ##EQU5## and the total noise resulting from the addition of two noise voltage levels is defined by the following equation: ##EQU6## wherein Vn1 is a first noise voltage level and Vn2 is a second noise voltage level. Total noise power Pnt is defined by:
Pnt =20 log Vnt +13.01 (7)
For example, the noise power in the output of the oscillator 2 coupled to the first of two inputs of the phase detector 3 which operates at 1 MHz is -160 dBc/Hz.
As is well known, the loop in which the phase detector 3 is located requires that the noise power in the signal applied to the second input of the phase detector 3 be equal to the noise power in the signal applied to the first input, i.e. -160 dBc/Hz. Working backward through the divider 4 and recognizing that if divider 4 was ideal, i.e. noise free, the noise power in the signal applied to its input would be higher by a factor of 20 log N, wherein N is the divisor. Thus, the noise power Pin at the input of the divider 4 would be given by the following equation:
Pin =noise power at output+20 log N (8)
where N=the divisor. For example, if the noise power in the output of divider 4 is -160 dBc/Hz, the noise power in its input would be calculated as follows: ##EQU7##
However, divider 4, like all conventional dividers, is not an ideal, noise free divider, but rather is also a source of noise. That is to say, the divider has a process dependent noise floor which depends on how it was made. For example, as indicated above, if the divider comprises a T2 L circuit having a maximum operating frequency of approximately 100 MHz, it will have a noise floor of -160 dBc/Hz. If the divider is made using Motorola emitter coupled logic (MECL) technology having a maximum operating frequency of approximately 600 MHz, it will have a noise floor of -150 dBc/Hz. On the other hand, if the divider is made using gallium arsenide (GaAs) it will have a maximum operating frequency of approximately 3000 megahertz (MHz), i.e. 3 gigahertz (GHz) and a noise floor of -130 dBc/Hz.
Since dividers are not ideal, when calculating backward to determine the actual noise power in the input of a divider which produces a given noise power in its output, it is necessary to add the noise power at the input as if the divider were ideal to the noise floor of the divider, as follows: ##EQU8##
For dBc/Hz=-150, (divider noise) (18)
Vn1 =10-8.15 (21)
Vn1 =7.07×10-9 (22)
(Vn1)2 =5.00×10-17 (23)
For dBcHz=-124.4, (theoretical noise in input) (24) ##EQU9##
Vn2 =10-6.87 (26)
Vn2 =1.35×10-7 (27)
(Vn2)2 =1.8233 10-14 (28)
Adding the two noise powers, one obtains: ##EQU10##
Pnt =20 log Vnt +13.01 dBc/Hz (32)
Pnt =124.39 dBc/Hz (actual noise in input) (33)
Similarly:
For dBc/Hz=-140, (theoretical noise in input) (34) ##EQU11##
Vn3 =10-7.65 (36)
Vn3 =2.236×10-8 (37)
(Vn3)2 =5×10-16 (38)
Adding the two noise powers Vn1 and Vn3, one obtains: ##EQU12##
Pnt =20 log Vnt +13.01 dBc/Hz (41)
Pnt =139.59 dBc/Hz (actual noise in input) (42)
Using the same techniques described above for calculating the noise power at the input of the mixer 11 and the prescaler 10, it will be found that the noise power is just slightly less than the noise power at the output of the mixer 11. That is to say, when the calculations are performed and the noise floor of the oscillator 12 is added to the noise power at the output of the mixer 11 as indicated in equations (33) and (42) above, it will be found that the sum of the noise powers is from -139.21 dBc/Hz to -121.37 dBc/Hz.
Calculating the noise power at the output of the prescaler 10 wherein the prescaler 10 divides the frequency of its input signal by a factor of 2, it will be found that if the prescaler 10 were ideal, the noise power at the output of the prescaler 10 would be reduced by a factor of 20 log P or 6 dBc/Hz to provide a theoretical noise power of 127.37 dBc/Hz to -145.21 dBc/Hz. However, because of the -150 dBc/Hz noise floor of the prescaler 10, using the above-described equations for calculating the actual noise power including the noise floor, it will be found that the actual noise power at the output of the prescaler 10 is -127.35 dBc/Hz to 143.97 dBc/Hz.
Referring to FIG. 2, the noise power in the high frequency input signal FRF to the sampler 15, which is also the noise power in the output signal having the frequency FO, is a function of the harmonic number of the sampler 15 which, as shown in FIG. 1, ranges from 8 to 82. As is well known in samplers, the noise is multiplied by the harmonic number H. Thus, the noise in the high frequency input and consequently in the output signal having the frequency FO wherein 20 log 8=18 dBc/Hz and 20 log 82=38.3 dBc/Hz, ranges from -112 dBc/Hz to -127 dBc/Hz for H=8 and from -92 dBc/Hz to -107 dBc/Hz for H=82, as shown in FIG. 2.
As indicated above, the output frequency for the circuit of FIG. 1 is given by an equation of the following general form: ##EQU13##
Referring to FIG. 3, there is provided in accordance with the present invention an ultra low phase noise microwave synthesizer designated generally as 50. In the synthesizer 50 there is provided an oscillator 51 for providing an output signal having a frequency Fstep, e.g. 10 MHz. The oscillator 51 has a noise floor of -160 dBc/Hz. The output of the oscillator 51 is coupled to the sampling input FS of a first harmonic sampler 52 and a first frequency input F1 of a first frequency presteer circuit F, also designated 53. The intermediate frequency output of the sampler 53 designated FIF is coupled to a first input of a summing circuit 55. The output IO of the first presteer circuit 53 is coupled to a second input of the summing circuit 55. The output IO of the summing circuit 55 is coupled to the control voltage input of a voltage-controlled oscillator (VCO) 54. The output of the VCO 54 is coupled to the high frequency input designated FRF of the sampler 52, to a second frequency input F2 of the first presteer circuit 53, to the high frequency input designated FRF of a second harmonic sampler 60 and to a first frequency input F1 of a second presteer circuit 61. As will be further described below, the first presteer circuit 53 is also provided with an input designated N1 for receiving a control signal corresponding to a multiplier for multiplying the frequency Fstep by a factor of from 60 to 118 for controlling the frequency Fidle of the VCO 54 over the frequency range of from 600 MHz to 1180 MHz.
The output of the second sampler 60 designated FIF and the output IO of the second presteer circuit 61 are coupled to a summing circuit 62. The output of the circuit 62 is coupled to a polarity control circuit 63. Circuit 63 having an output designated POL2 is responsive to a control signal from a circuit 69 for controlling the 10 polarity of the output of the summing circuit 62, i.e. inverting (-) and not inverting (+) said output, applied to the voltage-controlled oscillator 64. The VCO 64 provides an output having a frequency Fcoarse which ranges from 908.3 MHz to 983.3 MHz.
The output of the VCO 64 is coupled to one input of a mixer 65 and the input of a programmable divider 70. A second input of the mixer 65 is coupled to a source of a first reference frequency Fref1, e.g. 1000 MHz, i.e. 1 GHz, and a second reference frequency Fref2, e.g. 900 MHz. In practice, the frequencies Fref1 and Fref2 are obtained by multiplying the frequency, e.g. 100 MHz, of the output of an oscillator 66 by a factor of 10 and 9, respectively, using multipliers 67 and 68. The oscillator 66 has a noise floor of -165.
In practice, the output of the mixer 65 is restricted to a frequency range of from 8.3 MHz to 50 MHz by selecting between reference frequencies Fref1 and Fref2 and by controlling the polarity of the output POL2 of the polarity circuits 63 as a function of frequency Fcoarse. Thus, when Fcoarse ≧950 MHz, Fref1 and POL2(-) are selected and when Fcoarse <950 MHz, Fref2 and POL2(+) are selected.
The output of the mixer 65 is coupled to the sampling input FS of the second sampler 60 and to a second frequency input F2 of the second presteer circuit 61. As will be further described below, the second presteer circuit 61 is also provided with an input R for receiving a control signal corresponding to a divisor for dividing the frequency Fidle by a factor of from 12 to 96 for controlling, in conjunction with the sampler 52, the polarity circuit 63, the mixer 65, the summing circuit 55 and the source of reference frequencies Fref1 and Fref2, the frequency Fcoarse of the VCO 64 over the frequency range of 908.3 MHz to 983.3 MHz. As indicated above, the selection of the reference frequencies Fref1 and Fref2 and the polarity of the output of the circuit 63 depends on the frequency Fcoarse.
The programmable divider 70 has a pair of inputs designated SA and SB and is programmed to divide by 1, 2 or 4. The output of the divider 70 is coupled to the sampling input designated FS of a harmonic sampler 80. In conjunction with the operation of the system the sampler 80 operates over a range of harmonic numbers of from 8 to 23. The intermediate frequency output designated FIF of the sampler 80 is coupled to one input of a phase detector 81. A second input of the phase detector 81 is coupled to an oscillator 82. The oscillator 82, which has a noise floor of -160 dBc/Hz, provides an output having a frequency Ffine which ranges from 30 MHz to 40 MHz in response to a control signal Ffine. The output of the phase detector 81 is coupled to a voltage-controlled oscillator 83 by means of a polarity control circuit 84 having an output designated POL1 which is responsive to a control signal from a source 85 for controlling the polarity of the signal from the phase detector 81 applied to the VCO 83, i.e. for inverting (-) or not inverting (+) the signal. The output of the VCO 83 provides the output signal of the synthesizer 50 having a frequency FO of from 2 GHz to 20 GHz and is coupled to the high frequency input designated FRF of the sampler 80.
To provide a selected output frequency FO, a computer programmed in accordance with the listing shown in the appendix attached hereto and incorporated herein, is used to generate the control signals, N1, R, POL1, POL2 and P and to select the reference frequencies Fref1 and Fref2, such that the output frequency FO is given by the following equations: ##EQU14##
The values of P and H for each of three bands of frequencies is given below:
2G≦FO ≦5.1875G P=4, H=8-21 (48)
5.1875G<FO≦ 10.86G P=2, H=11-23 (49)
10.86G<FO ≦20G P=1, H=12-21 (50)
In general, P is chosen by the computer so that the harmonic number H of the sampler 80 is kept as low as possible.
Referring to FIG. 4, over the frequency range of interest, the worst case noise performance of the circuit of FIG. 3 is from -130.6 dBc/Hz at 2 GHz to -116.1 dBc/Hz at 20 GHz, or an improvement of from 18.6 dBc/Hz at 2 GHz to 24.1 dBc/Hz at 20 GHz over the noise performance of the prior known synthesizer of FIG. 1.
The circuits for generating the frequencies Fidle and Fcoarse comprise novel circuits for frequency multiplication and division, respectively, such as those disclosed in applicant's copending application Ser. No. 08/051,624, filed Apr. 22, 1993, entitled ULTRA LOW NOISE FREQUENCY DIVIDER/MULTIPLIER, the contents of which are incorporated herein by reference.
Referring to FIGS. 5 and 6, there is provided a multiplication circuit 100 and a division circuit 101, respectively. As more fully described in said application, each of the multiplication and division circuits 100 and 101 comprises a harmonic sampler 102, a presteer circuit 103, a summing circuit 104 and a VCO 105. The presteer circuit 103 comprises a pair of identical prescalers 110 and 111 and a programmable divider 112.
In the operation of each of the circuits 100 and 101 the harmonic sampler 102 is used to phase lock the VCO 105 to a frequency. However, due to the fact that the intermediate frequency FIF of a sampler can phase lock a VCO to any harmonic or subharmonic of the frequency applied to its sampling input, something else is required to drive the VCO to a predetermined frequency. To accomplish this, the presteer circuit 103 is used to compare the frequency applied to the sampling input of the sampler 102 with the frequency of the VCO 105 and, in response to a control signal corresponding to the desired VCO frequency, drive the VCO 105 to the desired frequency. Once the VCO 105 is at the desired frequency, the output of the presteer circuit 103 ceases to control the VCO frequency and it becomes phase locked thereto by the intermediate frequency FIF of the sampler 102.
Referring to FIG. 7, the operation of the division circuit comprising the sampler 60 and presteer circuit 61 is substantially the same as described above with respect to the circuit 101, except that the polarity circuit 63, mixer 65 and reference frequency source 66 are interposed in the VCO 64 voltage control and output circuits to offset the output frequency Fcoarse of the VCO 64 from a fraction of the frequency Fidle to a much higher frequency, e.g. 908.3 MHz to 983.3 MHz, thereby reducing the harmonic number of the following harmonic sampler 80.
To determine the noise performance of the circuit of FIG. 3, and specifically the noise power in the output of the mixer 65, a ratio of the frequency range of 8.3 MHz to 50 MHz at the output of the mixer 65 and the frequency Fstep, e.g. 10 MHz, of the oscillator 51 is calculated and found to extend from 8.3/10 to 50/10, or a value of 0.83 to 5∅ For frequencies wherein the ratio is less than 1, the circuits comprising the VCO's 54 and 64 operate as a divider. When the ratio is greater than 1, the circuits operate as a multiplier. Recognizing that the noise power in the output of the mixer 65 will be reduced or increased proportionately and using the above-described formula for calculating noise power, e.g. Pn =20 log N dBc/Hz, where N is a divisor or a multiplier, the noise power in the signal at the output of the mixer 65 relative to the noise power in the output of the oscillator 51 is calculated as follows:
20 log 0.83=-1.62 dBc/Hz (51)
20 log 5=14 dBc/Hz (52)
Adding these noise figures to the noise floor of the oscillator 51, it will be found that the noise power in dBc/Hz in the output of the mixer 65 ranges from a low of -161.60 (-160-1.62) to a high of -146 (-160+14).
Given that the noise power in the output of the mixer ranges from -161.6 dBc/Hz to -146 dBc/Hz and that the noise power in the reference signals Fref1 and Fref2 applied to one of the mixer inputs ranges from -145 dBc/Hz to -145.9 dBc/Hz, respectively, the noise power in the output of the VCO 64 and thus in the input to the programmable divider 70 can be calculated by adding the noise powers together as follows.
Using the general equation ##EQU15## and calculating the noise voltage levels in each reference signal, one obtains
V-145 =1.26×10-8 (54)
V-145.9 =1.13×10-8 (55)
and at the maximum and minimum frequencies FD, one obtains
V-161.6 =1.85×10-9 (56)
V-146 =1.12×10-8 (57)
Adding each of the noise voltage levels together using the general equations ##EQU16##
Pnt =20 log Vnt +13.01 (59)
one obtains the following:
Vnt (V-145 +V-161.6)=1.27×10-8 (60)
Pnt =144.9 (61)
Vnt (V-145 +V-146)=1.69×10-8 (62)
Pnt =-142.5 (63)
Vnt (V-145.9 +V-161.6)=1.15×10-8 (64)
Pnt =-145.8 (65)
Vnt (V-145.9 +V-146)=1.59×10-8 (66)
Pnt =-142.96 (67)
From the foregoing, it can be seen that the maximum and minimum noise powers in the input to the programmable divider 70 ranges from a low of -145.8 dBc/Hz to a high of -142.5 dBc/Hz.
The importance of using the two reference frequencies Fref1 and Fref2 in conjunction with the polarity circuit 63 to provide Fcoarse and keep the frequency at the output of the mixer 65 within the range of 8.3 MHz to 50 MHz with a relatively low noise power over that range, e.g. -161.6 dBc/Hz to -146 dBc/Hz, becomes evident when the noise figures are calculated using only one of the reference frequencies. For example, if only reference frequency Fref1, i.e. 1000 MHz, is used, the frequency FD at the output of the mixer 65 would range from 16.7 MHz to 91.7 MHz. Calculating the ratio of the frequency FD to the frequency Fstep, one obtains the following: ##EQU17##
Using the equation 20 log N and algebraically adding the result to the noise floor -160 dBc/Hz of the oscillator 51, the noise power at the minimum and maximum frequency FD in the output of the mixer 65 is then calculated as follows:
20 log 1.67=4.45 dBc/Hz (70)
-160 dBc/Hz+4.45 dBc/Hz=-155.6 dBc/Hz (71)
20 log 9.71=19.74 dBc/Hz (72)
-160 dBc/Hz+19.74 dBc/Hz=-140.3 dBc/Hz (73)
Adding the noise power of -145 dBc/Hz in the reference frequency Fref1 applied to one input of the mixer 65 to the above calculated noise powers in the output of the mixer 65, one obtains the noise powers in the signal applied to the second input of the mixer 65, which corresponds to the frequency Fcoarse, as follows: ##EQU18## where dBc/Hz is the noise floor in the reference signal having the frequency Fref1. From equations (70) and (72) above:
V1=V-145 =1.26×10-8 (75)
V2 =V-155.6 =3.71×10-9 (76)
V3 =V-140.3 =2.16×10-8 (77) ##EQU19##
Vnt =2.19×10-8 (79)
Pnt =20 log Vnt +13.01 (80)
Pnt =-144.6 dBc/Hz (81) ##EQU20##
Vnt =2.5×10-8 (83)
Pnt =-139 dBc/Hz (84)
Referring to the following comparison, it can be seen that if only Fref1 is used to generate Fcoarse, the noise power in the output of the VCO 64 is increased by more than 6 dBc/Hz. ##EQU21##
The above analysis shows that the noise performance is also reduced when the reference frequency is restricted to Fref2 of 900 MHz. Thus, using equations (74) and (78) above, a noise floor of -145.9 dBc/Hz for the reference signal and a frequency range of from 8.3 MHz (983.3-900) to 83.3 MHz (983.3-900), the following is calculated: ##EQU22##
20 log 0.83=-1.61 (87)
20 log 8.33=18.4 (88)
-160-1.61=-161.6 (89)
-160-18.4=-141.6 (90)
V-161.6 =1.85×10-9 (91)
V-141.6 =1.89×10-8 (92)
V-145.9 =1.13×10-8 (93)
Vnt (V-145.9 +V-161.6)=1.15×10-8 (94)
Pnt =145.8 dBc/Hz (95)
Vnt (V-145.9 +V-141.6)=2.18×10-8 (96)
Pnt =140.2 (97)
Comparing the above results with the results using two reference frequencies, it can be seen that the noise power in the output of the VCO 64 is increased by more than 3 dBc/Hz. ##EQU23##
Operating at 908.3 MHz to 983.3 MHz the divider 70 comprises MECL technology having a noise floor of -150 dBc/Hz. To calculate the noise power in the output signal of the divider 70, the divider output noise power due to dividing the noise power in the input signal by the divisor 1, 2 or 4 is decreased by the noise floor of the divider. This can be calculated by algebraically adding the two together as described above, such that the noise power in the output signal has the value shown in the following table for each value of P.
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P = 1 P = 2 P = 4 |
______________________________________ |
-142.5 -146.2 -148.7 |
-145.8 -147.5 -149.2 |
______________________________________ |
Referring to FIG. 4, given the above values of the noise power in the signal applied to the sampling input FS of the sampler 70 and the harmonic number of the sampler 70 derived by the computer program for selected output frequencies FO, the noise power in the output signal FO for various values of H and P at the selected frequencies can be calculated and have the following values: ##EQU24##
While a preferred embodiment of the present invention is described above, it is contemplated that numerous modifications may be made thereto for particular applications without departing from the spirit and scope of the present invention. Accordingly, it is intended that the embodiments described be considered only as illustrative of the present invention and that the scope thereof should not be limited thereto but be determined by reference to the claims hereinafter provided.
__________________________________________________________________________ |
APPENDIX |
__________________________________________________________________________ |
10 REM - ULPNALG - DAB 01/18/92 - ULTRA LOW PHASE NOISE MICROWAVE > |
20 REM - SYNTHESIZER ALGORITHM - |
30 REM - ULPNALG USES A 1,2,4 PRESCALER BETWEEN THE LO AND THE SAMPLER. |
- |
40 REM - THE PURPOSE IS TO REDUCE THE HARMONIC NUMBER OF THE SAMPLER > |
50 REM - FROM 8 THRU 23. THE COARSE LOOP IS NOW A SUMMING LOOP WITH A - |
60 REM - DIVIDE BY H DRIVING IT. THE DIVIDE BY H INPUT IS A 80 MHz TO > |
70 REM - 1180 MHz 10 MHz RESOLUTION SYNTHESIZER. THE ACTUAL SYNTHESIZER > |
9 |
80 REM - IS A 600 MHz TO 1180 MHz LOOP FOLLOWED BY A DIV/1,2,4,8. - |
90 REM - THE DIV/H AND DIV/L ARE COMBINED INTO A DIV/R, (DIV/R=DIV/H*1). |
- |
100 |
REM - THE RESULTS LEAD TO A -130.6 TO -116.1 dBC/Hz @ 10 KHz OFFSET > |
110 |
REM - AT 2 AND 20 GHz RESPECTIVLY. - |
120 |
CLS :KEY OFF |
130 |
INPUT "INPUT F(MHz)";FI# |
140 |
IF FI#<2000 OR FI#>20000 THEN PRINT " (2 TO 20 GHz)": GOTO 130 |
150 |
F1#=INT(.5+FI#*100000000#)/100000000#:REM - .01 Hz RESOLUTION - |
160 |
REM - CALCULATE SAMPLER LO FOR 30 TO 40 MHz IF - |
170 |
P=4 :REM - SAMPLER LO PRESCALER=4, IF=37.5-40 MHz - |
180 |
IF F1#>5187.5 THEN P=2 :REM - SAMPLER PRESCALER=2. IF=35-40 MHz - |
190 |
IF F1#>10860 THEN P=1 :REM - SAMPLER PRESCALER=1, IF=30-40 MHz - |
200 |
F=10*INT(F1#*P/10)/P :REM - INPUT FREQUENCY SCALED TO SAMPLER LO |
RESOLUTION - |
210 |
H1=1+INT(P*(F-43)/980) :REM - SAMPLER HARMONIC # FOR (+) POLARITY - |
220 |
H2=1+INT(P*(F+31)/980) :REM - SAMPLER HARMONIC # FOR (-) POLARITY - |
230 |
P1=H2-H1 :REM - SAMPLER MIX POLARITY 0=-, 1=+ |
240 |
ENPOL=0, POL=- M - YIG LOOP POLARITY - ENPOL=1, POL=+ |
250 |
P2=40-10*Pl*(8-(1/P)) :REM - SUM LOOP FREQUENCY SHIFT FOR POLARITY |
REVERSAL, 40 MHZ FOR (-) POLARITY, -30,-35,-37.5 FOR (+) POLARITY - |
260 |
F19=(F+P2)/H1 :REM - SAMPLER LO - |
270 |
F20=P*FI9 :REM - SUM LOOP FREQUENCY, DIV/P INPUT - |
280 |
F13=F20-900 :EN900=1 : REM - SUM LOOP INPUT USING 900 MHz OFFSET, |
POLARITY (+) - |
290 |
IF F20>950 THEN F13=1000-F20 :EN900=0 :REM - SUM LOOP INPUT USING 1000 |
MHz |
OFFSET, POLARITY (-) - |
300 |
REM - CALCULATE EXACT FREQUENCIES GIVEN 10 MHz RESOLUTION SUM LOOP |
SYNTHESIZER COVERING 80 TO 1180 MHz - |
310 |
F14#=10#*INT(.5+H1*F13/10) :REM - RECALCULATE DIV/H INPUT TO 10 MHz |
RESOLUTION USING HIGH PRECISION - |
320 |
REM - DETERMINE DIV/L VALUE 1,2,4 OR 8 - |
330 |
L=8 :REM - 80 TO 140 MHz - |
340 |
IF F14#>141 THEN L=4 :REM - 150 TO 290 MHz - |
350 |
IF F14#>291 THEN L=2 :REM - 300 TO 590 MHz - |
360 |
IF F14#>591 THEN L=1 :REM - 600 TO 1180 MHz - |
370 |
H#=INT(H1+.5) :L#=INT(L+.5) : P#=INT(P+.5) :REM - CONVERT TO HIGH |
PRECISION |
380 |
F15#=F14#/H#:REM - NEW SUM LOOP INPUT - |
390 |
F16#=1000#-FI5#:REM - NEW FLO USING 1000 MHz OFFSET - |
400 |
IF EN900=1 THEN F16#=900#+F15#:REM - NEW FLO USING 900 MHz OFFSET - |
410 |
N%=F14#*L#/10#:REM - Nl USED FOR 600 TO 1180 MHz SYNTHESIZER - |
420 |
R%=H#*L.#:REM - R USED FOR H*L DIVIDER - |
430 |
P%=P#:REM - P USED FOR SAMPLER PRESCALER - |
440 |
FS#=F16#/P#:REM - NEW SAMPLER LO FREQUENCY - |
450 |
F17#=ABS(H#*FS#-F1#) :REM - SAMPLER IF OUTPUT - |
460 |
F18#=INT(.5+100000000#*FI7#)/100#REM - SAMPLER IF OUTPUT .01 Hz |
RESOLUTION |
FINE LOOP REFERENCE FREQUENCY - |
470 |
480 |
PRINT " Fo(MHz) F-fine-(Hz) P R N1 POL1 POL2 |
" |
490 |
PRINT "---------------------------------------------------------------- |
----------------------- |
500 |
POL1$="-":POL2$="-" |
__________________________________________________________________________ |
INPUT F(MHz)? |
2000 |
Fo(MHz) Ffine(Hz) |
P R N1 POL1 |
POL2 |
2000.00000000 |
37500000.00 |
4 32 |
60 + - |
INPUT F(MHz)? |
2000.00000001 |
Fo(MHz) Ffine(Hz) |
P R N1 POL1 |
POL2 |
2000.00000001 |
37500000.01 |
4 32 |
60 + - |
INPUT F(MHz)? |
12345.67891234 |
Fo(MHz) Ffine(Hz) |
P R N1 POL1 |
POL2 |
12345.67891234 |
34321087.66 |
1 13 |
62 - - |
INPUT F(MHz)? |
19999.99999999 |
Fo(MHz) Ffine(Hz) |
P R N1 POL1 |
POL2 |
19999.99999999 |
30000000.01 |
1 21 |
97 - - |
INPUT F(MHz)? |
20000 |
Fo(MHz) Ffine(Hz) |
P R N1 POL1 |
POL2 |
20000.00000000 |
40000000.00 |
1 21 |
96 - - |
INPUT F(MHz)? |
2000 |
Fo(MHz) Ffine(Hz) |
P R N1 POL1 |
POL2 |
2000.00000000 |
35700000.00 |
4 32 |
60 + - |
INPUT F(MHz)? |
2000.00000001 |
Fo(MHz) Ffine(Hz) |
P R N1 POL1 |
POL2 |
2000.00000001 |
37500000.01 |
4 32 |
60 + - |
INPUT F(MHz)? |
12345.67991234 |
Fo(MHz) Ffine(Hz) |
P R N1 POL1 |
POL2 |
12345.67891234 |
34321087.66 |
1 13 |
62 - - |
INPUT F(MHz)? |
19999.99999999 |
Fo(MHz) Ffine(Hz) |
P R N1 POL1 |
POL2 |
19999.99999999 |
30000000.01 |
1 21 |
97 - - |
INPUT F(MHz)? |
20000 |
Fo(MHz) Ffine(Hz) |
P R N1 POL1 |
POL2 |
20000.00000000 |
40000000.00 |
1 21 |
96 - - |
__________________________________________________________________________ |
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Executed on | Assignor | Assignee | Conveyance | Frame | Reel | Doc |
May 10 1993 | BRADLEY, DONALD A | Wiltron Company | ASSIGNMENT OF ASSIGNORS INTEREST SEE DOCUMENT FOR DETAILS | 006555 | /0520 | |
May 12 1993 | Wiltron Company | (assignment on the face of the patent) | / | |||
Oct 01 1997 | Wiltron Company | Anritsu Company | CHANGE OF NAME SEE DOCUMENT FOR DETAILS | 010052 | /0559 |
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